Hostname: page-component-586b7cd67f-dsjbd Total loading time: 0 Render date: 2024-11-23T19:12:29.679Z Has data issue: false hasContentIssue false

Tree structure of spectra of spectral Moran measures with consecutive digits

Published online by Cambridge University Press:  22 December 2023

Cong Wang
Affiliation:
School of Mathematical Sciences, Henan Institute of Science and Technology, Xinxiang 453003, P. R. China e-mail: [email protected]
Feng-Li Yin*
Affiliation:
School of Mathematics and Statistics, Zhoukou Normal University, Zhoukou 466001, P. R. China
Rights & Permissions [Opens in a new window]

Abstract

Let $\{b_n\}_{n=1}^{\infty }$ be a sequence of integers larger than 1. We will study the harmonic analysis of the equal-weighted Moran measures $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ with ${\mathcal D}_n=\{0,1,2,\ldots ,q_n-1\}$, where $q_n$ divides $b_n$ for all $n\geq 1.$ In this paper, we first characterize all the maximal orthogonal sets of $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}})$ via a tree mapping. By this characterization, we give some sufficient conditions for the maximal orthogonal set to be an orthonormal basis.

Type
Article
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of Canadian Mathematical Society

1 Introduction

Let $\mu $ be a compactly supported Borel probability measure on ${\mathbb R}^d$ . We say that $\mu $ is a spectral measure if there exists a countable set $\Lambda $ of ${\mathbb R}^d$ such that $E(\Lambda )=\{e^{2\pi i \langle \lambda , x\rangle }:\lambda \in \Lambda \}$ forms an orthonormal basis for $L^2(\mu )$ . In this case, $\Lambda $ is called a spectrum of $\mu .$ Spectral theory for the Lebesgue measure on sets has been studied extensively since it is initialed by Fuglede in 1974 [Reference Fuglede16].

There exist probability measures that are not the restriction of the Lebesgue measure to bounded sets, but they admit spectra. In 1998, Jorgensen and Pedersen [Reference Jorgensen and Pedersen18] constructed the first example of a singular, non-atomic spectral measure $\mu _{4,\{0,2\}}$ (i.e., the one-fourth standard Cantor measure) and proved that the set

$$ \begin{align*}\Lambda=\Big\{\sum_{k=0}^n4^kd_k:d_k\in\{0,1\},n\geq 0\Big\}\end{align*} $$

is a spectrum of $\mu _{4,\{0,2\}}$ . Following this discovery, more interesting spectral measures were found and new spectra for $\mu _{4,\{0,2\}}$ were found (see [Reference An and He2, Reference Dai5, Reference Dai, Fu and Yan6, Reference Dai and Sun8, Reference Dutkay, Han and Sun10, Reference Łaba and Wang19, Reference Li20]). Subsequently, some singular phenomena different from the spectral theory of Lebesgue measures were discovered. For example, there exists only one spectrum with containing $0$ for $L^2[0,1]$ , while a given singular spectral measure $\mu $ has more than one spectrum which is not obtained by the translations of each other [Reference Dutkay, Han and Sun10, Reference Fu, He and Wen14]. Another surprising and interesting difference is that the Fourier expansions of functions in $L^2(\mu _{4,\{0,2\}})$ with respect to different spectra may have different convergence properties. Strichartz [Reference Strichartz22, Reference Strichartz23] proved that for any continuous function on ${\mathbb R}$ , its Fourier expansion with respect to $\Lambda $ is uniformly convergent; but Dutkay et al. showed in [Reference Dutkay, Han and Sun11] that there exists a continuous function on ${\mathbb R}$ whose Fourier expansion with respect to the spectrum $17\Lambda $ is divergent at $0$ . Based on the above exotic phenomena, a natural question is raised:

For a given spectral measure, can we find all spectra?

It is quite challenging to “characterize” all the spectra (no example is known with this property). Motivated by the above problem, many researchers concentrated their work on investigating self-similar/self-affine/Moran spectral measures and the construction of their spectra from various aspects (see [Reference An, Fu and Lai1, Reference An and Wang3, Reference Chen, Liu and Wang4, Reference Dai, He and Lai7Reference Dutkay, Han and Sun10, Reference Dutkay and Haussermann12, Reference Fu, He and Wen14, Reference Hu and Lau17, Reference Lu, Dong and Liu21, Reference Yan25] and the references therein).

Nowadays, there are a few of literature on this topic to construct new spectra. Most of this literature deals with the issue of self-similar/self-affine measures. Various of new spectra have been constructed for the measure $\mu _{4,\{0,2\}}$ by Dutkay et al. [Reference Dutkay, Han and Sun10], for self-similar measure with consecutive digits by Dai et al. [Reference Dai, He and Lai7], Dai [Reference Dai5], for infinite Bernoulli convolution by Li [Reference Li20], Fu et al. [Reference Fu, He and Wen14], for certain self-affine measures on ${\mathbb R}^d$ by Deng et al. [Reference Deng, Dong and Li9], etc. Besides these results, some answers for spectral Moran measures have been given in [Reference Fu and Wang15, Reference Wang and Yin24]. Motivated by these, the main focus of this paper is to study the classification of spectra of the so-called Moran measures with consecutive digits, where $\mu _{4,\{0,2\}}$ and Cantor measures with consecutive digits are special cases.

Let $\{b_n\}_{n=1}^{\infty }$ be a sequence of integers larger than 1 and ${\mathcal D}_{n}=\{0,1,2,\ldots ,q_n-1\}$ for each $n\geq 1,$ there exists a Borel probability measure $\mu _{\{b_n\},\{{\mathcal D}_n\}},$ which is defined by the following infinite convolutions of finite measures:

(1.1) $$ \begin{align} \mu_{\{b_n\},\{{\mathcal D}_n\}}=\delta_{b_1^{-1}{\mathcal D}_1}\ast\delta_{({b_1b_2})^{-1}{\mathcal D}_2}\ast \ldots, \end{align} $$

where $rE=\{rx:x\in E\},~\delta _E=\frac {1}{\#E}\sum _{e\in E}\delta _e$ ( $\#E$ is the cardinality of the finite set $E,~\delta _e$ is the Dirac measure at the point $e\in {\mathbb R}$ ) and the convergence is in a weak sense. Note that ${\mathcal D}_n=\{0,1,2,\ldots ,q_n-1\}$ , we call the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ a Moran measure with consecutive digits. In particular, when $b_n=b$ and ${\mathcal D}_n=\{0,1,\ldots ,q-1\}:={\mathcal D}$ for all $n \in {\mathbb N}$ , then the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ is reduced to the self-similar measure $\mu _{b,{\mathcal D}}$ (see [Reference Falconer13]).

Let us first recall the known results on the spectrality of the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ . In the self-similar case, Dai, He, and Lai [Reference Dai, He and Lai7] showed that the measure $\mu _{b,{\mathcal D}}$ is spectral if and only if $q|b$ . Recently, An and He [Reference An and He2] proved that if $q_n|b_n$ for all $n\geq 1,$ then $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ is a spectral measure. Continuing the above research, the main goal of this paper is to investigate the structure of spectra for the Moran spectral measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ .

The starting point of our approach is to analyze the precise structure of the zero set of the Fourier transform $\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}$ , and then we introduce the maximal orthonormal sets, as candidates for the spectra of the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ . We shows that there is one-to-one correspondence between a maximal orthonormal set and a tree mapping (Theorem 1.2). More precisely, we decomposed the maximal orthonormal sets of the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ using ${{\mathcal C}_j}$ -adic expansion and put them into a labeling of the tree.

Definition 1.1 Let $b_n=q_nr_n$ for all $n\geq 1,$ we say that $\tau $ is a tree mapping if it is a map $\tau :{\mathcal D}_{0,*}\rightarrow {\mathbb Z}$ which satisfies:

(i) $\tau (0^{n})=0$ for all $n\geq 1,$

(ii) for all $n\geq 1,~\tau (\sigma _{1}\dots \sigma _n) \in (\sigma _{n}+q_n{\mathbb Z})\bigcap \{-1,0,1,\ldots ,q_nr_{n+1}-2\},$

(iii) for any word $\sigma \in {\mathcal D}_{0,n}(n\geq 1),$ there exists $\sigma '\in {\mathcal D}_{n,\infty }$ such that $\tau \big ((\sigma \sigma ')|_j\big )=0$ for all j sufficiently large.

Given a tree mapping $\tau $ , we define the following sets:

$$ \begin{align*} {\mathcal D}(\tau)\!=\!\big\{\sigma\!\in\!{\mathcal D}_{0,\infty}\!: \tau(\sigma\!\mid\!_{m})\!=\!0~\text{for all }~m~\text{large enough}\big\} \end{align*} $$

and

$$ \begin{align*} \Lambda(\tau)=\Big\{\sum_{k=1}^{\infty}\tau(\sigma|_{k})r_k b_1\dots b_{k-1}\big|\sigma\in{\mathcal D}(\tau)\Big\}. \end{align*} $$

It will play a special role in the following theorem, which gives a characterization of the maximal orthogonal set of $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}})$ .

Theorem 1.2 The set $\Lambda $ with $0\in \Lambda $ is a maximal orthonormal set of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ if and only if there exists a tree mapping $\tau $ such that $\Lambda =\Lambda (\tau )$ .

While a maximal orthonormal set is not necessarily a spectrum since it may lack of completeness in $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}}).$ So what we need to do is to investigate under what conditions on $\tau $ such that the set $ \Lambda (\tau )$ to be a spectrum for the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ . We first introduce a good path to ensure the above maximal orthogonal set $ E\big (\Lambda (\tau )\big )$ to be a complete set in $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}}).$

Theorem 1.3 Let $\{q_n,b_n\}_{n=1}^\infty $ be a sequence of positive integers larger than 1 with $q_n|b_n$ for all $n\in {\mathbb N}$ and $\sup _{n\geq 1}\{b_n\}<\infty $ . Let $\tau $ be a tree mapping of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ . Suppose there is a constant integer $N>0$ such that for any word $\sigma \in {\mathcal D}_{0,k}(k\geq 1),$ there exists $\sigma '\in {\mathcal D}_{k,\infty }$ such that $\sigma \sigma '\in {\mathcal D}(\tau )$ and one of the following two conditions is satisfied:

(i) $\tau \big ((\sigma \sigma ')|_{k+j}\big )=0~$ for all $j\geq 1;$

(ii) $\tau \big ((\sigma \sigma ')|_{k+j}\big )=0$ for all $1\leq j\leq n,\ \tau \big ((\sigma \sigma ')|_{k+n+1}\big )\in q_{k+n+1}{\mathbb Z}\backslash \{0\}$ and

(1.2) $$ \begin{align} \max\Big\{j\geq1:\tau\big((\sigma\sigma')|_{k+n+j}\big)\neq 0 \Big\}\leq N. \end{align} $$

Then $\Lambda (\tau )$ is a spectrum of $\mu _{\{b_n\},\{{\mathcal D}_n\}}.$

We remark that (1.2) shows that the efficient length of the word $\sigma \sigma '$ is uniformly bounded, that is to say, $\sigma '$ is crucial in the proof of the completeness. However, the length of $\sigma \sigma '$ i.e., $\max \Big \{j\geq 1:\tau \big ((\sigma \sigma ')|_{k+j}\big )\neq 0 \Big \}$ may be not uniformly bounded since it also depends on the choice of n in $0^n$ .

Next, we consider other digits that can be used for the base expansion of the integers in the candidate set $\Lambda $ , and give a sufficient condition when these will generate spectra for the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ .

Definition 1.4 We say that $\tau $ is a generalized tree mapping if it is a mapping $\tau :{\mathcal D}_{0,*}\rightarrow {\mathbb Z}$ , which satisfies:

(i) $\tau (\sigma _{1}\sigma _2\dots \sigma _{n})=0$ if $\sigma _n=0$ ;

(ii) $\tau (\sigma _{1}\sigma _2\dots \sigma _{n}) \in \sigma _{n}+q_n{\mathbb Z}$ if $\sigma _n \neq 0$ .

We say that $\sigma \in {\mathcal D}_{0,\infty }$ is a useful word about the generalized tree mapping $\tau $ if there exists an integer $\tau ^\diamond (\sigma )\in {\mathbb Z}$ satisfying

$$ \begin{align*}\tau^\diamond(\sigma)\equiv\sum_{k=1}^n\tau(\sigma|_k)r_kB_{k-1}\quad \pmod{r_{n+1}B_n}, \qquad \text{for all}\ n\ge 1.\end{align*} $$

Given a generalized tree mapping $\tau $ , we let

$$ \begin{align*} \Lambda^\diamond(\tau)=\{\tau^\diamond(\sigma)|\sigma ~\text{is a useful word}\}. \end{align*} $$

Theorem 1.5 Let $\{q_n,b_n\}_{n=1}^\infty $ be a sequence of positive integers larger than 1 with $q_n|b_n$ for all $n\in {\mathbb N}$ and $\sup _{n\geq 1}\{b_n\}<\infty $ . Let $\tau $ be a generalized tree mapping,

(i) $\Lambda ^\diamond (\tau )$ is a maximal orthogonal set of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ ;

(ii) if $\sup _{\sigma \in {\mathcal D}_{0,*}}|\tau (\sigma )|<\infty $ , then $\Lambda ^\diamond (\tau )$ is a spectrum of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ .

The paper is organized as follows. In Section 2, we recall some preliminary results on basic criterion for spectral measures to prove our main results in the sequel, and characterize all the maximal orthonormal sets $\Lambda $ for $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}})$ . Theorem 1.3 is proved in Section 3. In Section 4, the proof of Theorem 1.5 is given.

2 Preliminaries and maximal orthogonal set

In this section, we first give some necessary definitions and facts that we need in the proof of the main theorem. Subsequently, we characterize all the maximal orthogonal sets $\Lambda $ for $L^2(\mu _{\{b_n\},\{{\mathcal D}_n\}})$ via a tree mapping (see Definition 1.1).

2.1 A criterion for spectral measures

Let $\mu $ be a probability measure with compact support on ${\mathbb R}.$ As usual, we define the Fourier transform of the measure $\mu $ ,

(2.1) $$ \begin{align} \widehat{\mu}(\xi)=\int e^{-2\pi i \xi x}d\mu(x). \end{align} $$

A countable set $\Lambda \subseteq {\mathbb R}$ is called an orthonormal set/ maximal orthonormal set/spectrum, respectively, of $\mu $ if $E(\Lambda ):=\{e^{ 2\pi i\lambda x}:\lambda \in \Lambda \}$ is an orthonormal set/maximal orthogonal set/orthonormal basis, respectively, for $L^{2}(\mu ).$ It is easy to show that $\Lambda $ is an orthogonal set of $\mu $ if and only if $\widehat {\mu }(\lambda _{i}-\lambda _{j})=0$ for any $\lambda _{i}\neq \lambda _{j}\in \Lambda $ , which is equivalent to

$$ \begin{align*} (\Lambda-\Lambda)\setminus\{0\}\subseteq\mathcal{Z}(\widehat{\mu}), \end{align*} $$

where $\mathcal {Z}(f):=\{\xi :f(\xi )=0\}$ is the set of the roots of the function $f(\xi ).$

Combining (1.1) and (2.1), we can conclude that

$$ \begin{align*} \widehat{\mu}_{{\{b_n\},\{{\mathcal D}_n\}}}(\xi)=\prod_{j=1}^{\infty} M_{{\mathcal D}_j}\Big(\frac{\xi}{b_1b_2\dots b_j}\Big), \end{align*} $$

where

$$ \begin{align*} M_{{\mathcal D}_j}(\xi)=\dfrac{1}{q_j}\Big(1+e^{-2\pi i\xi}+\dots+e^{-2\pi i(q_j-1)\xi}\Big). \end{align*} $$

A direct calculation shows that

$$ \begin{align*}\mathcal{Z}(M_{{\mathcal D}_j})=\Big\{\frac{a}{q_j}:q_j\nmid a,~a\in{\mathbb Z}\Big\},\end{align*} $$

where $q_j\nmid a$ means that $q_j$ does not divide $a.$ Hence, the zero of $\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}$ is given by

(2.2) $$ \begin{align} \mathcal{Z}(\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}})=\bigcup_{j\geq1} \left\{r_jB_{j-1}a:a\in{\mathbb Z} ~ \text{and} ~q_j\nmid a \right\}, \end{align} $$

where $r_j=b_j/q_j$ for all $j\geq 1$ and $B_j=b_0b_1\cdots b_j$ with $b_0=1$ .

To this end, we introduce a fundamental criterion for spectral measures, which is a direct application of Stone–Weierstrass Theorem and Parseval’s identity. For any $\xi \in {\mathbb R}$ , denote

$$ \begin{align*}Q(\xi)=\sum_{\lambda\in\Lambda}|\widehat{\mu}(\xi+\lambda)|^2.\end{align*} $$

Theorem 2.1 [Reference Jorgensen and Pedersen18]

Let $\mu $ be a Borel probability measure with compact support on ${\mathbb R}$ , and let $\Lambda \subseteq {\mathbb R}$ be a countable subset. Then:

(i) $\Lambda $ is an orthonormal set of $\mu $ if and only if $Q(\xi )\le 1$ for any $\xi \in {\mathbb R};$

(ii) $\Lambda $ is a spectrum of $\mu $ if and only if $Q(\xi )\equiv 1$ for any $\xi \in {\mathbb R};$

(iii) $Q(\xi )$ is an entire function in the complex plane if $\Lambda $ is an orthogonal set of $\mu .$

2.2 Maximal orthogonal sets

We start with some notations for simplicity. Fix such an integer $n\geq 0,$ let

$$ \begin{align*}{\mathcal D}_{n,k}=\{\sigma_{n+1}\sigma_{n+2}\dots \sigma_{n+k}: \sigma_j\in {\mathcal D}_j, n+1\leq j\leq n+k\}\end{align*} $$

be the set of all words with length $k.$ We adopt that ${\mathcal D}_{n,*}=\bigcup _{k=1}^\infty {\mathcal D}_{n,k}\bigcup \{\emptyset \}$ is the set of all the finite words beginning with ${\mathcal D}_{n+1}$ and ${\mathcal D}_{n,\infty }=\{\sigma _{n+1}\sigma _{n+2}\ldots : \sigma _k\in {\mathcal D}_k, k\geq n+1 \}$ is the set of all the infinite words beginning with ${\mathcal D}_{n+1}$ . For any $\sigma =\sigma _{n+1}\sigma _{n+2}\dots \sigma _{n+k}\in {\mathcal D}_{n,*},$ we use $|\sigma |=k$ to be its length and $\sigma \mid _j:=\sigma _{n+1}\sigma _{n+2}\dots \sigma _{n+j}(1\leq j \leq |\sigma |).$ For any $\sigma \in {\mathcal D}_{n,*}$ and $\sigma '\in {\mathcal D}_{n',*}\bigcup {\mathcal D}_{n',\infty },$ the word $\sigma \sigma '$ is their nature conjunction. In particular, $\emptyset I=I$ and $0^\infty =000\dots .$

For simplicity, we set $b_0=1$ and $B_k=b_0b_1b_2\dots b_k$ for all $k\geq 1$ . Given a tree mapping $\tau $ , recall that

(2.3) $$ \begin{align} {\mathcal D}(\tau)=\big\{\sigma\in{\mathcal D}_{0,\infty}: \tau(\sigma\!\mid\!_{m})\!=\!0~\text{for all }~m~\text{large enough}\big\}. \end{align} $$

For any $\sigma \in {\mathcal D}(\tau )$ , we let

(2.4) $$ \begin{align} \tau(\sigma)=\sum_{k=1}^{\infty}\tau(\sigma|_{k})r_kB_{k-1} \quad \text{and} \quad \Lambda(\tau)=\{\tau(\sigma)|\sigma\in{\mathcal D}(\tau)\}, \end{align} $$

which plays a special role in Theorem 1.2.

Before giving a proof of Theorem 1.2, we give the following lemma.

Lemma 2.2 Let $\mathcal {C}_n=\{-1,0,1,\ldots ,q_nr_{n+1}-2\}$ and $\textbf {C}_n=\mathcal {C}_{1}\times \cdots \times \mathcal {C}_n$ for all $n\geq 1.$ Then for any $k\in {\mathbb Z}(k\neq 0),$ there exists a unique word $\sigma =\sigma _{1}\sigma _{2}\dots \sigma _n\in \textbf {C}_n$ with $\sigma _n\neq 0,$ such that

$$ \begin{align*}k=\sigma_{1}+\sigma_{2}r_2q_1+\cdots+\sigma_nr_nq_1b_2\dots b_{n-1}:=\pi(\sigma).\end{align*} $$

Moreover, if $k=0,$ then $\sigma =\sigma _{1}=0.$

Proof For any $k\in {\mathbb Z}$ and $|k|<q_1r_2,$ let

$$ \begin{align*} \sigma= \begin{cases} 1(-1),\qquad\qquad k=-(q_1r_2-1),\\ (q_1r_2+k)(-1),\quad-(q_1r_2-1)<k<0,\\ k, \qquad\qquad\qquad0\leq k<q_1r_2-1,\\ -11,\qquad\qquad\quad k=q_1r_2-1,\nonumber \end{cases} \end{align*} $$

then $k=\pi (\sigma ).$ When $|k|>q_1r_2,$ then k can be decomposed uniquely as $k=c_{1}+k_{1}q_1r_2,$ where $c_{1}\in {\mathcal C}_{1}.$ If $|k_{1}|<q_2r_3,$ then $k_{1}$ has to be decomposed as in the previous step. Otherwise, we further decompose $k_{1}$ in a similar way and we get $|k_n|<q_{n+1}r_{n+2}$ after finite number k steps. The expansion is unique since each decomposition is unique.

Now, we can give the proof of Theorem 1.2.

Proof of Theorem 1.2

Suppose $\Lambda =\Lambda (\tau )$ for some tree mapping $\tau .$ We show that it is a maximal orthogonal of $\mu _{\{b_n\},\{{\mathcal D}_n\}}.$ To see this, we firstly show the orthogonality of $\Lambda $ . Pick two distinct $\lambda ,\lambda '\in \Lambda ,$ by the definition of $\Lambda (\tau ),$ we can find $\sigma \neq \sigma '\in {\mathcal D}(\tau )$ such that

$$ \begin{align*}\lambda=\sum_{j=1}^{\infty}\tau(\sigma|_{j})r_jB_{j-1}\quad \text{and}\quad \lambda'=\sum_{j=1}^{\infty}\tau(\sigma'|_{j})r_jB_{j-1}.\end{align*} $$

Let k be the first index such that $\sigma |_{k}\neq \sigma '|_{k}.$ Then, for some integer $M,$ we can write

$$ \begin{align*}\lambda-\lambda'=r_kB_{k-1}\Big(\tau(\sigma|_{k})-\tau(\sigma'|_{k})+Mq_{k}\Big).\end{align*} $$

By (ii) in Definition 1.1, $\tau (\sigma |_{k})$ and $\tau (\sigma '|_{k})$ are in distinct residue classes of $q_k.$ This implies $\lambda -\lambda ' \in \mathcal {Z}(\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}})$ and then $\Lambda (\tau )$ is orthogonal.

With respect to the maximality of the orthogonal set $\Lambda ,$ the proof is by contradiction. Suppose $\theta \in {\mathbb R}\backslash \Lambda $ and $\theta $ is orthogonal to all elements in $\Lambda .$ Since $0\in \Lambda $ , it gets that $\theta =\theta -0\in \mathcal {Z}(\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}).$ Hence, by (2.2), there exists $k\in {\mathbb Z}$ such that $\theta =r_kB_{k-1}a,$ where $a\in {\mathbb Z}$ and $q_k$ does not divide $a.$ By Lemma 2.2, it yields that

$$ \begin{align*}a=\epsilon_k+\epsilon_{k+1}q_kr_{k+1}+\dots+ \epsilon_{k+l}q_kr_{k+l}b_{k+1}b_{k+2}\dots b_{k+l-1},\end{align*} $$

where $\epsilon _{j}\in {\mathcal C}_{j}(k\leq j\leq k+l)$ and $q_k$ does not divide $\epsilon _{k}.$ Consequently, it can infer that

$$ \begin{align*}\theta=r_kB_{k-1}a=\epsilon_kr_kB_{k-1}+\epsilon_{k+1}r_{k+1}B_k+\cdots+ \epsilon_{k+l}r_{k+l}B_{k+l-1}.\end{align*} $$

Note that there exists unique $\sigma _{s}(0\leq \sigma _{s}\leq q_s-1)$ such that

$$ \begin{align*}\epsilon_{s}\equiv\sigma_{s}(\mathrm{mod}~q_s) \quad \forall~1\leq s\leq k+l.\end{align*} $$

Denote $\epsilon _{s}=\sigma _{s}=0$ for all $s>k+l.$ Since $\theta \notin \Lambda ,$ we can find the smallest integer $\alpha $ such that $\tau (\sigma _{1}\dots \sigma _{\alpha })\neq \epsilon _{\alpha }.$ By (iii) in the definition of $\tau ,$ we can find

$$ \begin{align*}\lambda=\sum_{j=1}^{\alpha}\tau(\sigma|_j)r_jB_{j-1}+MB_\alpha\end{align*} $$

for some integer $M.$ Then there exists $M'$ such that

$$ \begin{align*}\theta-\lambda=r_\alpha B_{\alpha-1} \Big(\epsilon_{\alpha}-\tau(\sigma|_{\alpha})+M'q_{\alpha}\Big).\end{align*} $$

By (ii) in the definition of $\tau ,~\tau (\sigma |_{\alpha })\equiv \sigma _{\alpha }~(\mathrm {mod}~q_\alpha ),$ which is also congruent to $\epsilon _{\alpha }$ by our construction. This implies $\theta -\lambda $ is not in the zero set of $\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}$ since $q_\alpha \mid \big (\epsilon _{\alpha }-\tau (\sigma |_{\alpha })\big ).$ It contradicts to $\theta $ being orthogonal to all $\lambda \in \Lambda .$

Conversely, suppose we are given a maximal orthogonal set $\Lambda $ of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ with $0\in \Lambda .$ Then $\Lambda \subset \mathcal {Z}(\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}).$ Hence, we expand $\lambda /r_1~(\lambda \in \Lambda )$ with Lemma 2.2 and get

(2.5) $$ \begin{align} \lambda=\sum_{j=1}^{k}\epsilon_{\lambda,j}r_jB_{j-1}: =\sum_{j=1}^{\infty}\epsilon_{\lambda,j}r_jB_{j-1}, \end{align} $$

where $\epsilon _{\lambda ,j}\in {\mathcal C}_j(1\leq j\leq k)$ with $\epsilon _{\lambda ,k}\neq 0$ and $\epsilon _{\lambda ,j}=0$ for all $j\geq k+1.$ Note that all $\epsilon _{0,n}$ are zero. We first consider $\epsilon _{\lambda ,1}$ the first coefficients of $\lambda $ ’s. As $\epsilon _{\lambda ,1}$ can be written uniquely as $i_k+q_1\alpha _k\in {\mathcal C}_1$ for some $i_k\in {\mathcal D}_1=\{0,1,\ldots ,q_1-1\},$ we claim that

$$ \begin{align*} \{\epsilon_{\lambda,1}\}_{\lambda\in\Lambda}=\{i+q_1\alpha_i: i \in{\mathcal D}_1\} \subseteq{\mathcal C}_1. \end{align*} $$

(Here $\alpha _i$ depends only on i but not on $\lambda ,$ hence the set has $q_1$ elements.) In fact, the orthogonality of $\Lambda $ implies that $\{\epsilon _{\lambda ,1}\}_{\lambda \in \Lambda }\subseteq \{i+q_1\alpha _i:i\in {\mathcal D}_1\}$ . On the other hand, if $\{\epsilon _{\lambda ,1}\}_{\lambda \in \Lambda }\subsetneqq \{i+q_1\alpha _i:i\in {\mathcal D}_1\},$ then there exists $0\leq i'\leq q_1-1$ such that $q_1\nmid (\epsilon _{\lambda ,1}-i')$ for all $\lambda \in \Lambda ,$ which contradicts the maximality of $\Lambda .$ This proves the claim.

From the claim, we can define $\tau $ on ${\mathcal D}_{0,1}$ by $\tau (\sigma _1)=\sigma _1+q_1\alpha _{\sigma _1}(\sigma _1\in {\mathcal D}_1)$ and in particular $\tau (0)=0.$ Similarly, we can show, for each $0\leq i_1\leq q_1-1,$ that

$$ \begin{align*}\{\epsilon_{\lambda,2}:\epsilon_{\lambda,1}=i_1+q_1\alpha_{i_1}\}_{\lambda\in\Lambda} =\{i_2+q_2\alpha_{i_2}:i_2\in{\mathcal D}_2\}\subseteq{\mathcal C}_2\end{align*} $$

and define $\tau (\sigma _1\sigma _2)=\sigma _2+q_2\alpha _{\sigma _2} (\sigma _2\in {\mathcal D}_2).$ Inductively, we can define a mapping $\tau $ on ${\mathcal D}_{0,*}$ . By the construction of $\tau ,$ it is easy to see that (i) and (ii) in Definition 1.1 are satisfied. For any $\sigma =\sigma _1\sigma _2\dots \sigma _m\in {\mathcal D}_{0,*},$ again by the construction of $\tau ,$ there exist infinitely many $\lambda $ such that $\epsilon _{\lambda ,t}=\sigma _t+q_t\alpha _{\sigma _t}$ for $1\leq t\leq m.$ Together with (2.5), fix such a k, if $m\geq k,$ then we have $\lambda =\sum _{j=1}^{\infty }\epsilon _{\lambda ,j}r_jB_{j-1} =\tau (\sigma 0^\infty );$ If $m< k,$ there exists $\sigma '=\sigma _{m+1}\sigma _{m+2}\dots \sigma _k$ such that $\epsilon _{\lambda ,n}=\tau (\sigma _1\dots \sigma _m\sigma _{m+1}\dots \sigma _n)$ for all $m+1\leq n\leq k.$ Then

$$ \begin{align*}\lambda=\sum_{j=1}^{\infty}\epsilon_{\lambda,j}r_jB_{j-1} =\tau(\sigma\sigma'0^\infty).\end{align*} $$

This implies that (iii) in Definition 1.1 holds. Hence, $\tau $ is a tree mapping and $\Lambda \subset \Lambda (\tau ).$ Conversely, $\Lambda (\tau )\subset \Lambda $ since $\Lambda $ is a maximal orthogonal set. And then $\Lambda =\Lambda (\tau ).$

3 The proof of Theorem 1.3

Theorem 1.2 shows that a countable set is a maximal orthonormal set of the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ if and only if it can be labeled as a tree. In this section, we will give a sufficient condition for a tree mapping to generate a spectrum. In the remainder of this paper, we always assume that the measure $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ satisfies $P=\sup _{n\geq 1}\{b_n\}<\infty $ . Given a tree mapping $\tau $ for $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ , we recall that

$$ \begin{align*}{\mathcal D}(\tau)=\big\{\sigma\in{\mathcal D}_{0,\infty}: \tau(\sigma\!\mid\!_{m})\!=\!0~\text{for all }~m~\text{large enough}\big\}\end{align*} $$

and

$$ \begin{align*}\tau(\sigma)=\sum_{k=1}^{\infty}\tau(\sigma|_{k})r_kB_{k-1},\quad \forall~\sigma\in{\mathcal D}(\tau),\end{align*} $$

where $B_n=b_0b_1\dots b_n$ with $b_0=1$ . Similarly, for any $\sigma '\in {\mathcal D}_{0,n}$ , we define

$$ \begin{align*}\tau^*(\sigma')=\sum_{k=1}^{n}\tau(\sigma'|_{k})r_kB_{k-1}.\end{align*} $$

We list some propositions, which will be useful in the sequel. Recall that

$$ \begin{align*}\mu_{\{b_n\},\{{\mathcal D}_n\}}(\cdot)&=\delta_{b_1^{-1}{\mathcal D}_1}\ast\delta_{({b_1b_2})^{-1}{\mathcal D}_2}\ast\dots\\&=\mu_n(\cdot)\ast\mu_{>n}(b_1b_2\dots b_n \cdot), \end{align*} $$

where $\mu _n$ is the convolutional product of the first n discrete measures and

$$ \begin{align*}\mu_{>n}=\delta_{b_{n+1}^{-1}{\mathcal D}_{n+1}}\ast \delta_{({b_{n+1}b_{n+2}})^{-1}{\mathcal D}_{n+2}}\ast\dots.\end{align*} $$

Proposition 3.1 Let $\tau $ be a tree mapping. Then, for any $\xi \in {\mathbb R}$ and for any $\sigma \in {\mathcal D}(\tau ),$ we have

$$ \begin{align*}\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}}\Big(\xi+\tau(\sigma)\Big) =\lim_{k\rightarrow\infty}\widehat{\mu}_k\Big(\xi+\tau^*(\sigma|_k)\Big).\end{align*} $$

Proof Since

$$ \begin{align*}\tau(\sigma)=\sum_{j=1}^{\infty}\tau(\sigma|_j)r_jB_{j-1} =\tau^*(\sigma|_k)+\sum_{j=k+1}^{\infty}\tau(\sigma|_j)r_jB_{j-1},\end{align*} $$

it follows from the periodicity of $|M_{{\mathcal D}_{s}}( x)|$ that

$$ \begin{align*}\widehat{\mu}_k\Big(\xi+\tau(\sigma)\Big) =\prod_{s=1}^kM_{{\mathcal D}_s}\Big(\xi+\tau(\sigma)\Big) =\prod_{s=1}^kM_{{\mathcal D}_s}\Big(\xi+\tau^*(\sigma|_k)\Big) =\widehat{\mu}_k\Big(\xi+\tau^*(\sigma|_k)\Big).\end{align*} $$

And then the result follows.

Proposition 3.2 Let $\tau $ be a tree mapping. Then, for all $k\in {\mathbb N}$ , we have

$$ \begin{align*}{\mathcal D}_{0,k}=\{\sigma|_k:\sigma\in{\mathcal D}(\tau)\}.\end{align*} $$

Proof Clearly, $\{\sigma |_k:\sigma \in {\mathcal D}(\tau )\}\subset {\mathcal D}_{0,k}.$ Conversely, it follows from (iii) of Definition 1.1 that for any word $\sigma '\in {\mathcal D}_{0,k},$ there exists $\sigma "\in {\mathcal D}_{k,\infty }$ such that $\sigma '\sigma "\in {\mathcal D}(\tau ).$ This implies ${\mathcal D}_{0,k}\subseteq \{\sigma |_k:\sigma \in {\mathcal D}(\tau )\}$ since $(\sigma '\sigma ")|_k=\sigma '\in {\mathcal D}_{0,k}.$ Hence, we finish the proof.

Proposition 3.3 Let $\tau $ be a tree mapping. Then, for all $k\geq 1$ and for any $\xi \in {\mathbb R}$ , we have

$$ \begin{align*}\sum_{\sigma\in {\mathcal D}_{0,k}} \big|\widehat{\mu}_k\big(\xi+\tau^*(\sigma)\big)\big|^2\equiv1.\end{align*} $$

Proof We claim that $\{\tau ^*(\sigma )\}_{\sigma \in {\mathcal D}_{0,k}}$ is a spectrum of $L^{2}(\mu _k).$ We can then use Theorem 2.1 to conclude our lemma. Since this set has exactly $q_1q_2\dots q_k$ elements, we just need to show the mutual orthogonality.

For any two distinct words $\sigma ,\sigma '\in {\mathcal D}_{0,k}$ , we have

$$ \begin{align*}\tau^*(\sigma)=\sum_{j=1}^{k}\tau(\sigma|_j)r_jB_{j-1} \quad \text{and} \quad \tau^*(\sigma')=\sum_{j=1}^{k}\tau(\sigma'|_j)r_jB_{j-1}.\end{align*} $$

Let $s~(1\leq s\leq k)$ be the first index such that $\sigma |_s\neq \sigma '|_s$ . Then we can obtain that

$$ \begin{align*}\tau^*(\sigma)-\tau^*(\sigma')=r_sb:{s-1}\Big(\tau(\sigma|_s)- \tau(\sigma'|_s)+Mq_s\Big)\end{align*} $$

for some integer M. It follows from the periodicity of the exponential function $e^{-2\pi ix}$ that

$$ \begin{align*}M_{{\mathcal D}_s}\Big(\frac{\tau^*(\sigma)-\tau^*(\sigma')}{B_s}\Big)= M_{{\mathcal D}_s}\Big(\frac{\tau(\sigma|_s)-\tau(\sigma'|_s)}{q_s}\Big)=0,\end{align*} $$

where the last equation holds because (ii) in the definition of maximal mapping implies that $q_s$ does not divide $\tau (\sigma |_s)-\tau (\sigma '|_s)$ . Since

$$ \begin{align*}\widehat{\mu}_k(\xi)=\prod_{j=1}^k\Big|M_{{\mathcal D}_j}\Big(\frac{\xi}{B_j}\Big)\Big|,\end{align*} $$

it follows that $\widehat {\mu }_k\big (\tau ^*(\sigma )-\tau ^*(\sigma ')\big )=0$ . And thus the desired result follows.

We divide the proof of Theorem 1.3 into several lemmas.

Lemma 3.4 Assume that for any $1\leq j\leq t, c_{k+j}\in \{-1,0,1,\ldots ,q_{k+j}r_{k+j+1}-2\}$ satisfies

$$ \begin{align*}c_{k+1}\in q_{k+1}{\mathbb Z}\backslash\{0\}\quad\text{and}\quad c_{k+t}\neq0.\end{align*} $$

Let $|\xi |\leq r_{k+1}-1/q_k,~~ \eta _1=\xi /b_{k+1}$ and

$$ \begin{align*}\eta_n=\frac{1}{b_{k+n}}\Big(\eta_{n-1}+\frac{c_{k+n-1}}{q_{k+n-1}}\Big),\end{align*} $$

then one has

$$ \begin{align*}\frac{1}{P^{n+1}} \leq |\eta_n| \leq \frac{1}{q_{k+n}}\Big(1-\frac{1}{P^2}\Big),\end{align*} $$

for all $2 \leq n \leq t,$ where $P=\sup _{n\geq 1}\{b_n\}<\infty $ .

Proof With an easy calculation, it can infer that

$$ \begin{align*}\eta_n=\frac{\xi+c_{k+1}r_{k+1}+\sum_{j=2}^{n-1}c_{k+j}r_{k+j}b_{k+1}\dots b_{k+j-1}}{b_{k+1}\dots b_{k+n}},\quad \forall 2\leq n \leq t.\end{align*} $$

On the upper bound, it follows $c_{k+j}\in \{-1,0,1,\ldots ,q_{k+j}r_{k+j+1}-2\}$ for all $1\leq j\leq n$ , then

(3.1) $$ \begin{align} |\eta_n|&=\left|\frac{\xi+c_{k+1}r_{k+1}+\sum_{j=2}^{n-1}c_{k+j}r_{k+j}b_{k+1}\dots b_{k+j-1}}{b_{k+1}\dots b_{k+n}}\right| \nonumber \\ &\leq\frac{r_{k+1}\!-\!1/q_k\!+\!(q_{k+1}r_{k+2}\!-\!2)r_{k+1} +\!\cdots\!+(q_{k+n-1}r_{k+n}\!-\!2) r_{k+n-1}b_{k+1}\dots b_{k+n-2}}{b_{k+1}b_{k+2}\!\dots\! b_{k+n}} \nonumber \\ &\leq\frac{r_{k+n}b_{k+1}\dots b_{k+n-1}-r_{k+n-1}b_{k+1}\dots b_{k+n-2}}{b_{k+1}\dots b_{k+n}} \nonumber \\ &=\frac{1}{q_{k+n}}\Big(1-\frac{1}{q_{k+n-1}r_{k+n}}\Big) \leq \frac{1}{q_{k+n}}\Big(1-\frac{1}{P^2}\Big), \end{align} $$

where the last inequality holds since $P=\sup _{n\geq 1}\{b_n\}$ .

On the lower bound, for $\eta _1$ , a direct calculation shows that

$$ \begin{align*}|\eta_1|\leq \frac{1}{q_{k+1}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

For $\eta _2=\frac {1}{b_{k+2}} \left (\eta _{1} +\frac {c_{k+1}}{q_{k+1}} \right ),$ since

$$ \begin{align*}c_{k+1}\in q_{k+1}{\mathbb Z}\backslash\{0\}\quad \text{and} \quad c_{k+1}\in \{-1,0,1,\ldots,q_{k+1}r_{k+2}-2\},\end{align*} $$

it follows that

$$ \begin{align*} |\eta_2|\geq \frac{1}{b_{k+2}}\left( 1-\frac{1}{q_{k+1}}\Big(1-\frac{1}{P^2}\Big)\right)> \frac{1}{2P}\geq\frac{1}{P^3}. \end{align*} $$

For $\eta _3=\frac {1}{b_{k+3}} \left (\eta _{2} +\frac {c_{k+2}}{q_{k+2}} \right ),$ where $c_{k+2}\in \{-1,0,1,\ldots ,q_{k+2}r_{k+3}-2\},$ one has the following two cases:

(i) if $c_{k+2}=0$ , then $\eta _3=\frac {1}{b_{k+3}} \eta _{2}$ , and hence

$$ \begin{align*} |\eta_3|>\frac{1}{P^3b_{k+3}}\geq \frac{1}{P^4}; \end{align*} $$

(ii) if $c_{k+2} \not =0,$ then

$$ \begin{align*} |\eta_3|> \frac{1}{b_{k+3}} \left( \frac{1}{q_{k+2}}-\frac{1}{q_{k+2}}\Big(1-\frac{1}{P^2}\Big) \right)=\frac{1}{q_{k+2}b_{k+3}P^2}\geq \frac{1}{P^4}. \end{align*} $$

Noting that $\frac {1}{P^4}\leq \frac {1}{q_{k+3}}\Big (1-\frac {1}{P^2}\Big ).$ Then we get that

$$ \begin{align*}\frac{1}{P^{4}} \leq |\eta_3| \leq \frac{1}{q_{k+3}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

Continuing the above procedure several times, we can obtain, for all $2 \leq n \leq t$ , that

$$ \begin{align*}\frac{1}{P^{n+1}} \leq |\eta_n| \leq \frac{1}{q_{k+n}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

Hence, the lemma is proved.

Since $\sup _{n\geq 1}\{b_n\}<\infty $ and $q_n|b_n,$ there are only finitely many $(b_n,{\mathcal D}_n),$ say that $\big (b(1),{\mathcal D}(1)\big ),\ \big (b(2),{\mathcal D}(2)\big ),\ldots ,\big (b(N),{\mathcal D}(N)\big )$ with $D(i)=\{0,1,\ldots ,q_{(i)}-1\}$ for some $N\in {\mathbb N}.$ Hence, it is easy to show that

(3.2) $$ \begin{align} c_1=\min\left\{\big|M_{{\mathcal D}(i)}(\xi)\big|:|\xi|\leq \frac{1}{q_{(i)}}\Big(1-\frac{1}{P^2}\Big)\right\}>0, \end{align} $$

and

(3.3) $$ \begin{align} c(t)=\min\left\{\big|M_{{\mathcal D}(i)}\left(\xi+\frac{j}{q(i)}\right)\big|: \begin{array}{ll} \xi\in\! \left(\left[\! \frac{1}{P^{t+1}}, \frac{1}{q_{(i)}}\Big(1\!-\!\frac{1}{P^2}\Big)\!\right]\! \cup \!\left[\! \!-\!\frac{1}{q_{(i)}}\Big(1\!-\!\frac{1}{P^2}\Big),-\frac{1}{P^{t+1}}\!\right] \right)\\ \forall j\in \left\{0, 1,\dots, q(i)-1 \right\} \end{array} \right\}>0. \end{align} $$

The following lemma will be use to prove Lemma 3.6, which is crucial in proof of completeness of the maximal orthogonal set.

Lemma 3.5 Assume that for any $1\leq j\leq t, c_{k+j}\in \{-1,0,1,\ldots ,q_{k+j}r_{k+j+1}-2\}$ satisfies

$$ \begin{align*}c_{k+1}\in q_{k+1}{\mathbb Z}\backslash\{0\}\quad\text{and}\quad c_{k+t}\neq0.\end{align*} $$

Let $|\xi |\leq r_{k+1}-1/q_k$ , and let

$$ \begin{align*}\eta=\xi+c_{k+1}r_{k+1}+\sum_{j=2}^tc_{k+j}r_{k+j}b_{k+1}\dots b_{k+j-1},\end{align*} $$

then there exists a constant $C(t)\in (0,1)$ (only depending on t) such that $|\widehat {\mu }_{>k}(\eta )|\geq C(t).$

Proof We define $\eta _1=\frac {\xi }{b_{k+1}}$ and

$$ \begin{align*}\eta_n=\frac{\xi+c_{k+1}r_{k+1}+\sum_{j=2}^{n-1}c_{k+j}r_{k+j}b_{k+1}\dots b_{k+j-1}}{b_{k+1}\dots b_{k+n}},\quad \forall 2\leq n \leq t.\end{align*} $$

According to the fact that

$$ \begin{align*}\Big|\widehat{\mu}_{>k}(\eta)\Big|=\prod_{s=1}^\infty \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big|,\end{align*} $$

it follows from the periodicity of $|M_{{\mathcal D}_{k+s}}( x)|$ and $c_{k+1}\in q_{k+1}{\mathbb Z}\backslash \{0\}$ that

$$ \begin{align*} \Big|\widehat{\mu}_{>k}(\eta)\Big|=\Big|M_{{\mathcal D}_{k+1}}\Big(\eta_1\Big)\Big|\cdot \prod_{s=2}^{t}\Big|M_{{\mathcal D}_{k+s}}\Big(\eta_s+\frac{a_{k+s}}{q_{k+s}}\Big)\Big|\cdot \prod_{s=t+1}^{\infty}\Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big|, \end{align*} $$

where $a_{k+s} \equiv c_{k+s}~(\mathrm {mod}~q_{k+s})$ with $a_{k+s}\in \{0,1,\ldots ,q_{k+s}-1\}$ for $2\leq s\leq t.$

We estimate the products one by one. From the proof of Lemma 3.4, it can infer that

$$ \begin{align*}|\eta_1|\leq \frac{1}{q_{k+1}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

And thus we have, together with (3.2), that

(3.4) $$ \begin{align} \Big|M_{{\mathcal D}_{k+1}}\Big(\eta_1\Big)\Big|\geq c_1>0. \end{align} $$

For any $2\leq s\leq t$ , using Lemma 3.4 again, we also have that

$$ \begin{align*}\frac{1}{P^{s+1}} \leq |\eta_s| \leq \frac{1}{q_{k+s}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

It follows from (3.3) that

(3.5) $$ \begin{align} \Big|M_{{\mathcal D}_{k+s}}\Big(\eta_s+\frac{a_{k+s}}{q_{k+s}}\Big)\Big|\geq c(t)>0. \end{align} $$

For $s\geq t+1,$ we set

$$ \begin{align*}\gamma=\frac{\eta}{b_{k+1}\dots b_{k+t}}\end{align*} $$

for convenience. Thus, we conclude that

$$ \begin{align*}\Big|\frac{\gamma}{b_{k+t+1}}\Big|\leq \frac{1}{q_{k+t+1}}\Big(1-\frac{1}{P^2}\Big).\end{align*} $$

Using (3.2) again, it gets that

(3.6) $$ \begin{align} \prod_{s=t+1}^{\infty}\Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big| &=\Big|M_{{\mathcal D}_{k+t+1}}\Big(\frac{\gamma}{b_{k+t+1}}\Big)\Big|\cdot \prod_{m=2}^{\infty}\Big|M_{{\mathcal D}_{k+t+s}}\Big(\frac{\gamma}{b_{k+t+1}\dots b_{k+t+m}}\Big)\Big|\nonumber\\ &=\Big|M_{{\mathcal D}_{k+t+1}}\Big(\frac{\gamma}{b_{k+t+1}}\Big)\Big|\cdot \prod_{m=2}^{\infty} \Big|\frac{\sin q_{k+t+m}\pi\gamma (b_{k+t+1}\dots b_{k+t+m})^{-1}}{q_{k+t+m} \sin \pi \gamma (b_{k+t+1}\dots b_{k+t+m})^{-1}}\Big)\Big|\nonumber\\ &\geq c_1\cdot \prod_{m=2}^{\infty} \Big|\frac{\sin q_{k+t+m}\pi\gamma (b_{k+t+1}\dots b_{k+t+m})^{-1}}{q_{k+t+m} \pi \gamma (b_{k+t+1}\dots b_{k+t+m})^{-1}}\Big)\Big|. \end{align} $$

On the other hand, for any $m\geq 2$ , it can be easily checked that

$$ \begin{align*}\Big|\frac{q_{k+t+m}\pi\gamma}{b_{k+t+1}\dots b_{k+t+m}}\Big| \leq\frac{\pi(1-\frac{1}{P^2})}{q_{k+t+1}b_{k+t+2}\dots b_{k+t+m-1}r_{k+t+m}} \leq \frac{\pi(1-\frac{1}{P^2})}{2^{m-1}}.\end{align*} $$

Combined this with (3.6), we can obtain from the monotonicity of $|\sin x/x|$ in $[0,\pi ]$ and $\sin x/x\geq 1-6^{-1}x^2$ for $x\in [0,\pi /2]$ that

(3.7) $$ \begin{align} \prod_{s=t+1}^{\infty}\Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big|\geq c_1\cdot \prod_{m=1}^\infty \Big(1-\frac{\pi^2(1-\frac{1}{p^2})^2}{6\cdot 4^m}\Big):=c'>0. \end{align} $$

Combined with (3.4), (3.5), and (3.7), we get that

$$ \begin{align*}|\widehat{\mu}_{>k}(\eta)|\geq c_1c(t)^{t-1}c'>0.\end{align*} $$

Therefore, the desired result follows from $C(t)=c_1c(t)^{t-1}c'$ .

Lemma 3.6 For any word $\sigma \in {\mathcal D}_{0,k}(k\geq 1),$ let $\sigma \sigma '\in {\mathcal D}(\tau )$ satisfying (1.2) given as in Theorem 1.3. Let $|\xi |\leq r_{k+1}-1/q_k$ , and let

$$ \begin{align*}\eta=\xi+\frac{\sum_{j=1}^{\infty}\tau\big((\sigma\sigma')|_{k+j}\big)r_{k+j}B_{k+j-1}}{B_{k}}.\end{align*} $$

Then there exists a constant c such that $|\widehat {\mu }_{>k}(\eta )|\geq c.$

Proof We distinguish two cases to prove it.

Case I. When $\sigma '=0^\infty $ with $\tau \big ((\sigma \sigma ')|_j\big )=0$ for any $ j\geq k+1,$ thus $\eta =\xi $ and

$$ \begin{align*}|\eta|\leq r_{k+1}-\frac{1}{q_k}.\end{align*} $$

It is easy to check that $|\widehat {\mu }_{>k}(\eta )|\geq c'>0,$ where $c'$ is given as in (3.7).

Case II. When $\sigma '=0^n\delta (n\in {\mathbb N},\delta \in {\mathcal D}_{k+n,\infty })$ with $\tau \big ((\sigma \sigma ')|_{k+j}\big )=0~(\forall ~1\leq j\leq n),$

$$ \begin{align*} \tau\big((\sigma\sigma')|_{k+n+1}\big)\in q_{k+n+1}{\mathbb Z}\backslash\{0\} \quad \text{and} \quad \max\Big\{j:\tau\big((\sigma\sigma')|_{k+n+j}\big)\neq 0, ~~ j\geq1 \Big\}\leq N. \end{align*} $$

Together with the periodicity of $|M_{{\mathcal D}_{k+s}}( x)|$ , it implies that

(3.8) $$ \begin{align} |\widehat{\mu}_{>k}(\eta)|&=\prod_{s=1}^\infty \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big| \nonumber\\ &=\prod_{s=1}^{n} \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big|\cdot \prod_{s=n+1}^{\infty}\Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\eta}{b_{k+1}\dots b_{k+s}}\Big)\Big|\nonumber\\ &=\prod_{s=1}^{n} \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\xi}{b_{k+1}\dots b_{k+s}}\Big)\Big|\cdot |\widehat{\mu}_{>k+n}(\gamma)|, \end{align} $$

where

$$ \begin{align*}\gamma=\frac{\eta}{b_{k+1}\!\dots\! b_{k+n}}=\frac{\xi}{b_{k+1}\!\dots\! b_{k+n}} +\tau\big((\sigma\sigma')|_{k+n+1}\big)c_{k+n+1} +\!\sum_{j=2}^\infty\! \tau\big((\sigma\sigma')|_{k+n+j}\big)r_{k+n+j}b_{k+n+1}\!\dots b_{k+n+j-1}.\end{align*} $$

Since $\max \Big \{j:\tau \big ((\sigma \sigma ')|_{k+n+j}\big )\neq 0, ~~ j\geq 1 \Big \}\leq N$ , it follows that $\gamma $ can be rewritten as

$$ \begin{align*}\gamma=\frac{\xi}{b_{k+1}\!\dots\! b_{k+n}} +\tau\big((\sigma\sigma')|_{k+n+1}\big)c_{k+n+1} +\!\sum_{j=2}^N\! \tau\big((\sigma\sigma')|_{k+n+j}\big)r_{k+n+j}b_{k+n+1}\!\dots b_{k+n+j-1}.\end{align*} $$

Using Lemma 3.5, there exists a constant $C(N)\in (0,1)$ (only depending on N) such that

(3.9) $$ \begin{align} |\widehat{\mu}_{>k+n}(\gamma)|>C(N). \end{align} $$

Note that $|\xi |\leq r_{k+1}-1/q_k$ , we also have

(3.10) $$ \begin{align} \prod_{s=1}^{n} \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\xi}{b_{k+1}\dots b_{k+s}}\Big)\Big|\geq \prod_{s=1}^\infty \Big|M_{{\mathcal D}_{k+s}}\Big(\frac{\xi}{b_{k+1}\dots b_{k+s}}\Big)\Big|=|\widehat{\mu}_{>k}(\xi)|\geq c', \end{align} $$

where the last inequality holds from Case I.

Combined with (3.8), (3.9), and (3.10), we get that

$$ \begin{align*}|\widehat{\mu}_{>k}(\eta)|\geq C(N)c'>0.\end{align*} $$

Let $c=C(N)c'$ , we can obtain the desired result.

Now, we have all ingredients for the proof of Theorem 1.3.

Proof of Theorem 1.3.

Since $\tau $ is a tree mapping, it follows that $\Lambda (\tau )$ is a maximal orthogonal set. By Theorem 2.1, we have

$$ \begin{align*}Q(\xi)&=\sum_{I\in{\mathcal D}(\tau)}\Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(I)\Big)\Big|^2\\ &=\sum_{n=0}^\infty \sum_{I\in{\mathcal D}(\tau),l_{\tau}(I)=n}\Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(I)\Big)\Big|^2\leq1, \quad \forall~\xi\in{\mathbb R}.\end{align*} $$

Here, $l_{\tau }(I)$ is the smallest integer n such that $\tau (I|_k)=0$ for all $k\geq n$ . Moreover, fixed $\xi \in (0,1),$ for any $\epsilon>0,$ there exists an integer $N_\epsilon $ such that

(3.11) $$ \begin{align} \sum_{I\in{\mathcal D}(\tau),l_{\tau}(I)\geq N_\epsilon}\Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(I)\Big)\Big|^2<\epsilon. \end{align} $$

From Theorem 2.1, we only need to show that $Q(\xi )\geq 1$ for all $\xi \in (0,1).$ Together with Proposition 3.1, it can infer that

$$ \begin{align*} Q(\xi)&\geq \sum_{I\in{\mathcal D}(\tau),l_{\tau}(I)< N_\epsilon}\Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(I)\Big)\Big|^2\nonumber\\ &=\sum_{I\in{\mathcal D}(\tau),l_{\tau}(I)< N_\epsilon}\lim_{k\rightarrow\infty}\Big|\widehat{\mu}_{k} \Big(\xi+\tau^*(I|_k)\Big)\Big|^2\nonumber\\ &=\lim_{k\rightarrow\infty}\sum_{I'\in{\mathcal D}(\tau),l_{\tau}(I)< N_\epsilon}\Big|\widehat{\mu}_{k} \Big(\xi+\tau^*(I|_k)\Big)\Big|^2. \end{align*} $$

Using the condition of Theorem 1.3, it follows that

(3.12) $$ \begin{align} Q(\xi)&\geq \lim_{k\rightarrow\infty}\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')<N_\epsilon} \!\Big|\widehat{\mu}_{k} \Big(\xi+\tau^*\big((\sigma\sigma')|_k\big)\Big)\Big|^2 \nonumber\\ &=\lim_{k\rightarrow\infty}\!\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')<N_\epsilon} \Big|\widehat{\mu}_k \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2, \end{align} $$

where $\sigma '$ are given as in the theorem. It can easily be checked that

$$ \begin{align*} \Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(\sigma\sigma')\Big)\Big| &=\Big|\widehat{\mu}_k\Big(\xi+\tau^{*}(\sigma)\Big)\Big|\cdot \Big|\widehat{\mu}_{>k}\\ &\quad \Big(\frac{\xi+\tau^{*}(\sigma)}{B_k} \!+\frac{\sum_{j=1}^{\infty}\tau\big((\sigma\sigma')|_{k+j}\big)r_{k+j}B_{k+j-1}}{B_{k}}\Big)\Big|, \end{align*} $$

and

$$ \begin{align*} \Big|\frac{\xi+\tau^{*}(\sigma)}{B_k}\Big|=\Big|\frac{\xi+ \sum_{j=1}^k \tau(\sigma|_j)r_jB_{j-1}}{B_k}\Big| \leq r_{k+1}-\frac{1}{q_k}. \end{align*} $$

Therefore, combining with Lemma 3.6, we get

$$ \begin{align*} \Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau(\sigma\sigma')\Big)\Big| \geq c\Big|\widehat{\mu}_k\Big(\xi+\tau^{*}(\sigma)\Big)\Big|, \end{align*} $$

where c is given in Lemma 3.6. Together with (3.11), it yields that

$$ \begin{align*}\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')\geq N_\epsilon} \Big|\widehat{\mu}_k \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2 \leq\frac{1}{c^2}\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma') \geq N_\epsilon} \Big|\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}} \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2 <\frac{\epsilon}{c^2}.\end{align*} $$

Applying Propositions 3.2 and 3.3, we infer that

$$ \begin{align*} \sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')<N_\epsilon} \Big|\widehat{\mu}_k \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2+\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')\geq N_\epsilon} \Big|\widehat{\mu}_k \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2=1. \end{align*} $$

Then using (3.12), we obtain that

$$ \begin{align*} Q(\xi)\geq\lim_{k\rightarrow\infty} \Big(1-\sum_{\sigma\in{\mathcal D}_{0,k},l_\tau(\sigma\sigma')\geq N_\epsilon} \Big|\widehat{\mu}_k \Big(\xi+\tau^*\big(\sigma\big)\Big)\Big|^2\Big) \geq1-\frac{\epsilon}{c^2}. \end{align*} $$

Hence, $Q(\xi )\geq 1$ and this completes the proof of Theorem 1.3.

4 The proof of Theorem 1.5

The aim of this section is to prove Theorem 1.5. Recall that $\sigma \in {\mathcal D}_{0,\infty }$ is a useful word about the generalized tree mapping $\tau $ if there exists an integer $\tau ^\diamond (\sigma )\in {\mathbb Z}$ satisfying

$$ \begin{align*}\tau^\diamond(\sigma)\equiv\sum_{k=1}^n\tau(\sigma|_k)r_kB_{k-1} \quad\pmod{r_{n+1}B_n}, \qquad \text{for all}\ n\ge 1.\end{align*} $$

It is easy to see that if $\sigma \in {\mathcal D}_{0,\infty }$ is a useful word, then the associated $\tau ^\diamond (\sigma )$ is unique. Given a generalized tree mapping $\tau $ , we let

$$ \begin{align*} {\mathcal D}^\diamond(\tau)=\big\{\sigma\in{\mathcal D}_{0,\infty}: \sigma~\text{is a useful word}\big\} \quad \text{and} \quad \Lambda^\diamond(\tau)=\{\tau^\diamond(\sigma)|\sigma\in{\mathcal D}^\diamond(\tau)\}. \end{align*} $$

Proof of Theorem 1.5.

(i) We first show that $\Lambda ^\diamond (\tau )$ is an orthogonal set of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ . For any two distinct words $\sigma ,\sigma '\in {\mathcal D}^\diamond (\tau )$ , we let n be the first index such that $\sigma |_n \neq \sigma '|_n$ . Since

$$ \begin{align*}\tau^\diamond(\sigma)\equiv\sum_{k=1}^n\tau(\sigma|_k)r_kB_{k-1} \!\quad\pmod{r_{n+1}B_n} \quad\! \text{and}\! \quad \tau^\diamond(\sigma')\equiv\sum_{k=1}^n\tau(\sigma'|_k)r_kB_{k-1} \quad\pmod{r_{n+1}B_n},\end{align*} $$

it follows that

$$ \begin{align*}\tau^\diamond(\sigma)-\tau^\diamond(\sigma')=r_nB_{n-1}\Big(\tau(\sigma|_n)-\tau(\sigma'|_n)+q_nM\Big)\end{align*} $$

for some integer M. Using the definition of the generalized tree mapping, we know that

$$ \begin{align*}q_n\nmid \Big(\tau(\sigma|_n)-\tau(\sigma'|_n)\Big).\end{align*} $$

Together with (2.2), we also have that

$$ \begin{align*}\tau^\diamond(\sigma)-\tau^\diamond(\sigma')\in \mathcal{Z}(\widehat{\mu}_{\{b_n\},\{{\mathcal D}_n\}}).\end{align*} $$

Hence, $\Lambda ^\diamond (\tau )$ is an orthogonal set of $\mu _{\{b_n\},\{{\mathcal D}_n\}}$ .

Next, we show the maximality of $\Lambda ^\diamond (\tau )$ by contradiction. Suppose that there exists a $\theta \in {\mathbb R}\backslash \Lambda ^\diamond (\tau )$ such that $\theta $ is orthogonal to all elements in $\Lambda ^\diamond (\tau )$ . Note that $0\in \Lambda ^\diamond (\tau )$ , we have that $\theta \in \mathcal {Z}(\widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}})$ . Hence, by (2.2), there exists $k\in {\mathbb Z}$ such that $\theta =r_kB_{k-1}a,$ where $a\in {\mathbb Z}$ and $q_k$ does not divide $a.$ By Lemma 2.2, it yields that

$$ \begin{align*}a=\epsilon_k+\epsilon_{k+1}q_kr_{k+1}+\cdots+ \epsilon_{k+l}q_kr_{k+l}b_{k+1}b_{k+2}\dots b_{k+l-1},\end{align*} $$

where $\epsilon _{j}\in {\mathcal C}_{j}=\{-1,0,1,\ldots ,q_jr_{j+1}-2\}(k\leq j\leq k+l)$ and $q_k$ does not divide $\epsilon _{k}.$ Consequently, it can infer that

(4.1) $$ \begin{align} \theta=r_kB_{k-1}a=\epsilon_kr_kB_{k-1}+\epsilon_{k+1}r_{k+1}B_k+\cdots+ \epsilon_{k+l}r_{k+l}B_{k+l-1}, \end{align} $$

where $q_k$ does not divide $\epsilon _{k}.$ Note that there exists unique $\sigma _j~(0\leq \sigma _j\leq q_j-1)$ such that

$$ \begin{align*}\epsilon_j\equiv\sigma_j\quad\pmod{q_j} \quad \forall~k\leq j\leq k+l.\end{align*} $$

Denote $\sigma _j=0$ for all $1\leq j<k$ and let $\sigma =\sigma _1\sigma _2\dots \sigma _{k+l}$ . By the definition of useful words, it can be easily checked that $\sigma 0^\infty $ is a useful word.

Since $\theta \notin \Lambda ^\diamond (\tau ),$ we can find the smallest integer $\alpha $ such that $\tau (\sigma _{1}\dots \sigma _{\alpha })\neq \epsilon _{\alpha }.$ Hence,

$$ \begin{align*}\theta-\tau^\diamond(\sigma0^\infty)=r_\alpha B_{\alpha-1} \Big(\epsilon_{\alpha}-\tau\big((\sigma0^\infty)|_{\alpha}\big)+Mq_{\alpha}\Big),\end{align*} $$

for some integer M. Using the definition of the generalized tree mapping again, we know that $(\sigma 0^\infty )|_{\alpha }\equiv \sigma _{\alpha }~(\mathrm {mod}~q_\alpha ),$ which is also congruent to $\epsilon _{\alpha }$ by our construction. It implies that

$$ \begin{align*}q_\alpha\mid\Big(\epsilon_{\alpha}-\tau\big((\sigma0^\infty)|_{\alpha}\big)\Big),\end{align*} $$

and thus $\theta -\tau ^\diamond (\sigma 0^\infty )\notin \widehat {\mu }_{\{b_n\},\{{\mathcal D}_n\}}$ . This contradicts the assumption and the maximality of $\Lambda ^\diamond (\tau )$ follows.

(ii) Together with the conclusion (i) and Theorem 1.2, there exists a tree mapping $\tau _1$ such that $\Lambda ^\diamond (\tau )=\Lambda (\tau _1)$ . For any $\sigma '\in {\mathcal D}_{0,k}~(k\geq 1)$ , by the definition of the tree mapping $\tau _1$ , there is an infinite word $\sigma "\in {\mathcal D}_{k,\infty }$ such that $\sigma '\sigma "\in {\mathcal D}(\tau _1)$ . Since $\Lambda ^\diamond (\tau )=\Lambda (\tau _1)$ , it follows that there exists $\sigma \in {\mathcal D}^\diamond (\tau )$ such that $\tau ^\diamond (\sigma )=\tau _1(\sigma '\sigma ").$ Note that $\sigma |_k0^\infty $ is a useful word, we can find $\sigma "'\in {\mathcal D}(\tau _1)$ such that $\tau ^\diamond (\sigma |_k0^\infty )=\tau _1(\sigma "')$ . Hence, one has that

(4.2) $$ \begin{align} \tau_1(\sigma'\sigma")\equiv\tau^\diamond(\sigma)\equiv\tau^\diamond(\sigma|_k0^\infty)\equiv\tau_1(\sigma"')\quad \pmod{r_{n+1}B_n} \quad \text{for any} ~1\leq n\leq k. \end{align} $$

A direct calculation shows that

$$ \begin{align*}\mid\tau_1^*\big((\sigma'\sigma")|_n\big)-\tau_1^*(\sigma"'|_n)\mid\leq \sum_{j=1}^{n}(q_jr_{j+1}-2)r_jB_{j-1}<r_{n+1}B_n.\end{align*} $$

Together with (4.2), it implies that $\tau _1^*\big ((\sigma '\sigma ")|_n\big )=\tau _1^*(\sigma "'|_n)$ for all $1\leq n\leq k$ and thus we have that

$$ \begin{align*}\sigma"'|_k=(\sigma'\sigma")|_k=\sigma'.\end{align*} $$

Hence, we rewrite $\sigma "'$ as $\sigma "'=\sigma '\delta $ with $\delta \in {\mathcal D}_{k,\infty }$ . Since $\sup _{\sigma \in {\mathcal D}_{0,*}}|\tau (\sigma )|<\infty $ , there exists a constant M such that $|\tau (\sigma )|<2^M$ for all $\sigma \in {\mathcal D}_{0,*}$ . Then

(4.3) $$ \begin{align} |\tau_1(\sigma'\delta)|=|\tau^\diamond(\sigma|_k0^\infty)|\leq 2^M\sum_{j=1}^k r_jB_{j-1}\leq 2^{M+1}r_kB_{k-1}. \end{align} $$

Repeating the procedure of (4.1), we also have that

(4.4) $$ \begin{align} 2^{M+1} r_kB_{k-1}=\vartheta_kr_kB_{k-1}+\vartheta_{k+1}r_{k+1}B_k+\cdots+ \vartheta_{k+\ell}r_{k+\ell}B_{k+\ell-1}, \end{align} $$

where $\vartheta _j\in {\mathcal C}_j$ for all $k\leq j\leq k+\ell $ . Then it is easy to check that

$$ \begin{align*} 2^{M+1} r_kB_{k-1}&=|\vartheta_kr_kB_{k-1}+\vartheta_{k+1}r_{k+1}B_k+\cdots+ \vartheta_{k+\ell}r_{k+\ell}B_{k+\ell-1}|\\ &\geq r_{k+\ell}B_{k+\ell-1}-\sum_{j=k}^{k+\ell-1}(q_jr_{j+1}-2)r_jB_{j-1}\\ &\geq r_{k+\ell-1}B_{k+\ell-2}. \end{align*} $$

Consequently, it can infer that

$$ \begin{align*}2^{M+1}\geq r_{k+\ell-1}q_kb_{k+1}b_{k+2}\dots b_{k+\ell-2}\geq 2^{\ell-1},\end{align*} $$

and thus $\ell \leq M+2$ .

We let m be the largest order of the expansion of $\tau (\sigma '\delta )$ with respect to the base $\{{\mathcal C}_j\}_{j=1}^\infty $ . Using (4.3) and (4.4), it can obtain that

$$ \begin{align*}m\leq k+\ell \leq k+M+2.\end{align*} $$

Therefore, it follows from the definition of m that

$$ \begin{align*}\max\Big\{j\geq1:\tau_1\big((\sigma'\delta)|_{k+j}\big)\neq 0 \Big\}\leq M+2.\end{align*} $$

Hence, the conclusion (ii) follows form Theorem 1.3.

Footnotes

This work was supported by the National Natural Science Foundation of China (Grant No. 12101196) and the Natural Science Foundation of Henan Province (Grant No. 212300410323).

References

An, L. X., Fu, X. Y., and Lai, C. K., On spectral Cantor–Moran measures and a variant of Bourgain’s sum of sine problem . Adv. Math. 349(2019), 84124.10.1016/j.aim.2019.04.014CrossRefGoogle Scholar
An, L. X. and He, X. G., A class of spectral Moran measures . J. Funct. Anal. 266(2014), 343354.10.1016/j.jfa.2013.08.031CrossRefGoogle Scholar
An, L. X. and Wang, C., On self-similar spectral measures . J. Funct. Anal. 280(2021), 108821.10.1016/j.jfa.2020.108821CrossRefGoogle Scholar
Chen, M. L., Liu, J. C., and Wang, X. Y., Spectrality of a class of self-affine measures on ${\mathbb{R}}^2$ . Nonlinearity 34(2021), 74467469.10.1088/1361-6544/ac2493CrossRefGoogle Scholar
Dai, X. R., Spectra of Cantor measures . Math. Ann. 366(2016), 16211647.10.1007/s00208-016-1374-5CrossRefGoogle Scholar
Dai, X. R., Fu, X. Y., and Yan, Z. H., Spectrality of self-affine Sierpinski-type measures on ${\mathbb{R}}^2$ . Appl. Comput. Harmon. Anal. 52(2021), 6381.10.1016/j.acha.2019.12.001CrossRefGoogle Scholar
Dai, X. R., He, X. G., and Lai, C. K., Spectral property of Cantor measures with consecutive digits . Adv. Math. 242(2013), 187208.10.1016/j.aim.2013.04.016CrossRefGoogle Scholar
Dai, X. R. and Sun, Q. Y., Spectral measures with arbitrary Hausdorff dimensions . J. Funct. Anal. 268(2015), 24642477.10.1016/j.jfa.2015.01.005CrossRefGoogle Scholar
Deng, Q. R., Dong, X. H., and Li, M. T., Tree structure of spectra of spectral self-affine measures . J. Funct. Anal. 277(2019), 937957.10.1016/j.jfa.2019.04.006CrossRefGoogle Scholar
Dutkay, D., Han, D. G., and Sun, Q. Y., On spectra of a Cantor measure . Adv. Math. 221(2009), 251276.10.1016/j.aim.2008.12.007CrossRefGoogle Scholar
Dutkay, D., Han, D. G., and Sun, Q. Y., Divergence of the mock and scrambled Fourier series on fractal measures . Trans. Amer. Math. Soc. 366(2014), 21912208.10.1090/S0002-9947-2013-06021-7CrossRefGoogle Scholar
Dutkay, D. and Haussermann, J., Number theory problem from the harmonic analysis of a fractal . J. Number Theory 159(2016), 726.10.1016/j.jnt.2015.07.009CrossRefGoogle Scholar
Falconer, K. J., Fractal geometry, mathematical foundations and applications, Wiley, New York, 1990.Google Scholar
Fu, Y. S., He, X. G., and Wen, Z. X., Spectra of Bernoulli convolutions and random convolutions . J. Math. Pures Appl. 116(2018), 105131.10.1016/j.matpur.2018.06.002CrossRefGoogle Scholar
Fu, Y. S. and Wang, C., Spectra of a class of Cantor–Moran measures with three-element digit sets . J. Approx. Theory 261(2021), 105494.10.1016/j.jat.2020.105494CrossRefGoogle Scholar
Fuglede, B., Commuting self-adjoint partial differential operators and a group theoretic problem . J. Funct. Anal. 16(1974), 101121.10.1016/0022-1236(74)90072-XCrossRefGoogle Scholar
Hu, T. Y. and Lau, K. S., Spectral property of the Bernoulli convolution . Adv. Math. 219(2008), 554567.10.1016/j.aim.2008.05.004CrossRefGoogle Scholar
Jorgensen, P. and Pedersen, S., Dense analytic subspaces in fractal ${L}^2$ spaces. J. Anal. Math. 75(1998), 185228.Google Scholar
Łaba, I. and Wang, Y., On spectral Cantor measures . J. Funct. Anal. 193(2002), 409420.10.1006/jfan.2001.3941CrossRefGoogle Scholar
Li, J. L., Spectra of a class of self-affine measures . J. Funct. Anal. 260(2011), 10861095.10.1016/j.jfa.2010.12.001CrossRefGoogle Scholar
Lu, Z. Y., Dong, X. H., and Liu, Z. S., Spectrality of Sierpinski-type self-affine measures . J. Funct. Anal. 282(2022), 109310.10.1016/j.jfa.2021.109310CrossRefGoogle Scholar
Strichartz, R., Mock Fourier series and transforms associated with certain Cantor measures . J. Anal. Math. 81(2000), 209238.10.1007/BF02788990CrossRefGoogle Scholar
Strichartz, R., Convergence of mock Fourier series . J. Anal. Math. 99(2006), 333353.10.1007/BF02789451CrossRefGoogle Scholar
Wang, C. and Yin, F. L., Exponential orthonormal bases of Cantor–Moran measures . Fractals 27(2019), 1950136.10.1142/S0218348X19501366CrossRefGoogle Scholar
Yan, Z. H., Spectral Moran measures on ${\mathbb{R}}^2$ . Nonlinearity 35(2022), 12611285.10.1088/1361-6544/ac4a8aCrossRefGoogle Scholar